07 - balance principles. me338 - syllabus balance principles balance principles. cauchy s postulate. cauchy s lemma -t
|
|
- Quentin Ray
- 5 years ago
- Views:
Transcription
1 me338 - syllabus holzapfel nonlinear solid mechanics [2000], chapter 4, pages cauchy s postulate cauchy s lemma cauchy s postulate stress vector t to a plane with normal n at position x only depends on plane s normal n Px cauchy s lemma -t -n newton s third law actio = reactio n t 3 4
2 cauchy s theorem cauchy X 3, x 3 cauchy s postulate t 2 t t 1 X 2, x 2 stress vector t to a plane with normal n at position x only depends on plane s normal n cauchy s lemma X 1, x 1 t 3 cauchy s theorem newton s third law actio = reactio cauchy s theorem existence of second order tensor field σ is inde- pendent of n, such that t is a linear function of n existence of second order tensor field σ is inde- pendent of n, such that t is a linear function of n 5 6 illustration of stress components normal and tangential stress x 3 e 3 stress vector t n n t interpretation of 3x3 components normal stress t t e 2 x 2 tangential stress x 1 e 1 7 8
3 stress tensors cauchy / true stress relates spatial force to spatial area first piola kirchhoff / nominal stress relates spatial force to material area second piola kirchhoff stress relates material force to material area stress tensors cauchy / true stress relates spatial force to spatial area first piola kirchhoff / nominal stress relates spatial force to material area second piola kirchhoff stress relates material force to material area 9 10 stress tensors transport mechanisms covariant / strains first piola kirchhoff pull back push forward gustav robert kirchhoff [ ] second piola kirchhoff cauchy contravariant / stresses pull back push forward 11 12
4 of mass, momentum, angular momentum and energy, supplemented with an entropy inequality constitute the set of conservation laws. the law of conservation of mass/matter states that the mass of a closed system of substances will remain constant, regardless of the processes acting inside the system. the principle of conservation of momentum states that the total momentum of a closed system of objects is constant. of mass, linear momentum, angular momentum and energy apply to all material bodies. each one gives rise to a field equation, holing on the configurations of a body in a sufficiently smooth motion and a jump condition on surfaces of discontinuity. like position, time and body, the concepts of mass, force, heating and internal energy which enter into the formulation of the balance equations are regarded as having primitive status in continuum mechanics. chadwick continuum mechanics [1976] potato potato [1] isolate subset from [1] isolate subset from [2] characterize influence of remaining body through phenomenological quantities - contact fluxes, &
5 potato potato [1] isolate subset [2] characterize influence of remaining body through phenomenological quantities - contact fluxes, & [3] from define basic physical quantities - mass, linear and angular momentum, energy generic balance equation [1] isolate subset from [2] characterize influence of remaining body through phenomenological quantities - contact fluxes, & [3] define basic physical quantities - mass, linear and angular momentum, energy [4] postulate balance of these quantities here: closed systems general format balance quantity flux source production unlike open systems closed systems have a constant mass examples of open systems: rocket propulsion and biological growth (me337)
6 transformation of volume elements - determinant of mass is always constant and positive changes in volume - determinant of deformation tensor changes in volume and density are related through and mass is constant global material density is constant local
7 balance of (linear) momentum density no mass flux no mass source no mass production continuity equation linear momentum density momentum flux - stress momentum source - force no momentum production equilibrium equation compare balance of (internal) energy internal energy density heat flux heat source no heat production mass point energy equation internal mechanical power external thermal power
06 - concept of stress concept of stress concept of stress concept of stress. me338 - syllabus. definition of stress
holzapfel nonlinear solid mechanics [2000], chapter 3, pages 109-129 holzapfel nonlinear solid mechanics [2000], chapter 3, pages 109-129 1 2 me338 - syllabus definition of stress stress [ stres] is a
More information06 - kinematic equations kinematic equations
06 - - 06-1 continuum mechancis continuum mechanics is a branch of physics (specifically mechanics) that deals with continuous matter. the fact that matter is made of atoms and that it commonly has some
More informationELASTOPLASTICITY THEORY by V. A. Lubarda
ELASTOPLASTICITY THEORY by V. A. Lubarda Contents Preface xiii Part 1. ELEMENTS OF CONTINUUM MECHANICS 1 Chapter 1. TENSOR PRELIMINARIES 3 1.1. Vectors 3 1.2. Second-Order Tensors 4 1.3. Eigenvalues and
More informationChapter 3. Forces, Momentum & Stress. 3.1 Newtonian mechanics: a very brief résumé
Chapter 3 Forces, Momentum & Stress 3.1 Newtonian mechanics: a very brief résumé In classical Newtonian particle mechanics, particles (lumps of matter) only experience acceleration when acted on by external
More informationCourse Syllabus: Continuum Mechanics - ME 212A
Course Syllabus: Continuum Mechanics - ME 212A Division Course Number Course Title Academic Semester Physical Science and Engineering Division ME 212A Continuum Mechanics Fall Academic Year 2017/2018 Semester
More information4.3 Momentum Balance Principles
4.3 Momentum Balance Principles 4.3.1 Balance of linear angular momentum in spatial material description Consider a continuum body B with a set of particles occupying an arbitrary region Ω with boundary
More information02 - introduction to vectors and tensors. me338 - syllabus. introduction tensor calculus. continuum mechanics. introduction. continuum mechanics
02 - introduction to vectors and tensors me338 - syllabus holzapfel nonlinear solid mechanics [2000], chapter 1.1-1.5, pages 1-32 02-1 introduction 2 the potato equations is the branch of mechanics concerned
More information10 - basics constitutive equations - volume growth - growing tumors
10 - basics - volume growth - growing tumors 10 - basic 1 where are we??? balance equations balance equations balance equations of mass, momentum, angular momentum and energy, supplemented with an entropy
More informationChapter 3: Stress and Equilibrium of Deformable Bodies
Ch3-Stress-Equilibrium Page 1 Chapter 3: Stress and Equilibrium of Deformable Bodies When structures / deformable bodies are acted upon by loads, they build up internal forces (stresses) within them to
More informationThe Navier-Stokes Equations
s University of New Hampshire February 22, 202 and equations describe the non-relativistic time evolution of mass and momentum in fluid substances. mass density field: ρ = ρ(t, x, y, z) velocity field:
More informationMeasurement of deformation. Measurement of elastic force. Constitutive law. Finite element method
Deformable Bodies Deformation x p(x) Given a rest shape x and its deformed configuration p(x), how large is the internal restoring force f(p)? To answer this question, we need a way to measure deformation
More informationPhysical Conservation and Balance Laws & Thermodynamics
Chapter 4 Physical Conservation and Balance Laws & Thermodynamics The laws of classical physics are, for the most part, expressions of conservation or balances of certain quantities: e.g. mass, momentum,
More informationSpri ringer. INTERFACIAL TRANSPORT PHENOMENA 2 nd Edition. John C. Slattery Department ofaerospace Engineering Texas A&M University
INTERFACIAL TRANSPORT PHENOMENA 2 nd Edition John C. Slattery Department ofaerospace Engineering Texas A&M University Leonard Sagis Department of Agrotechnology & Food Science Wageningen University Eun-Suok
More informationGeometry for Physicists
Hung Nguyen-Schafer Jan-Philip Schmidt Tensor Analysis and Elementary Differential Geometry for Physicists and Engineers 4 i Springer Contents 1 General Basis and Bra-Ket Notation 1 1.1 Introduction to
More informationContinuum mechanics V. Constitutive equations. 1. Constitutive equation: definition and basic axioms
Continuum mechanics office Math 0.107 ales.janka@unifr.ch http://perso.unifr.ch/ales.janka/mechanics Mars 16, 2011, Université de Fribourg 1. Constitutive equation: definition and basic axioms Constitutive
More information04 - kinematic equations - large deformations and growth
04 - - large deformations and growth continuum mechancis is a branch of physics (specifically mechanics) that deals continuous matter. the fact that matter is made of atoms and that it commonly has some
More information07 - basics balance equations - closed and open systems
07 - basics - closed and open systems 07-1 where *are* we??? 2 final projects mechanically driven growth of skin: chris, adrian, xuefeng muscle growth: brandon, robyn, esteban, ivan, jenny cardiac growth
More informationLectures on. Constitutive Modelling of Arteries. Ray Ogden
Lectures on Constitutive Modelling of Arteries Ray Ogden University of Aberdeen Xi an Jiaotong University April 2011 Overview of the Ingredients of Continuum Mechanics needed in Soft Tissue Biomechanics
More informationDRIVING FORCE IN SIMULATION OF PHASE TRANSITION FRONT PROPAGATION
Chapter 1 DRIVING FORCE IN SIMULATION OF PHASE TRANSITION FRONT PROPAGATION A. Berezovski Institute of Cybernetics at Tallinn Technical University, Centre for Nonlinear Studies, Akadeemia tee 21, 12618
More information4 Constitutive Theory
ME338A CONTINUUM MECHANICS lecture notes 13 Tuesday, May 13, 2008 4.1 Closure Problem In the preceding chapter, we derived the fundamental balance equations: Balance of Spatial Material Mass ρ t + ρ t
More informationNonlinear Theory of Elasticity. Dr.-Ing. Martin Ruess
Nonlinear Theory of Elasticity Dr.-Ing. Martin Ruess geometry description Cartesian global coordinate system with base vectors of the Euclidian space orthonormal basis origin O point P domain of a deformable
More informationMITOCW MITRES2_002S10nonlinear_lec15_300k-mp4
MITOCW MITRES2_002S10nonlinear_lec15_300k-mp4 The following content is provided under a Creative Commons license. Your support will help MIT OpenCourseWare continue to offer high quality educational resources
More informationINDEX 363. Cartesian coordinates 19,20,42, 67, 83 Cartesian tensors 84, 87, 226
INDEX 363 A Absolute differentiation 120 Absolute scalar field 43 Absolute tensor 45,46,47,48 Acceleration 121, 190, 192 Action integral 198 Addition of systems 6, 51 Addition of tensors 6, 51 Adherence
More informationCourse No: (1 st version: for graduate students) Course Name: Continuum Mechanics Offered by: Chyanbin Hwu
Course No: (1 st version: for graduate students) Course Name: Continuum Mechanics Offered by: Chyanbin Hwu 2011. 11. 25 Contents: 1. Introduction 1.1 Basic Concepts of Continuum Mechanics 1.2 The Need
More informationin this web service Cambridge University Press
CONTINUUM MECHANICS This is a modern textbook for courses in continuum mechanics. It provides both the theoretical framework and the numerical methods required to model the behavior of continuous materials.
More informationChapter 2: Fluid Dynamics Review
7 Chapter 2: Fluid Dynamics Review This chapter serves as a short review of basic fluid mechanics. We derive the relevant transport equations (or conservation equations), state Newton s viscosity law leading
More informationNavier-Stokes Equation: Principle of Conservation of Momentum
Navier-tokes Equation: Principle of Conservation of Momentum R. hankar ubramanian Department of Chemical and Biomolecular Engineering Clarkson University Newton formulated the principle of conservation
More informationArmin Toffler, The whole is more than the sum of the parts. Aristotle, BC. Prigogine I. and Stengers I. Order out of Chaos (1984)
1 OUTLINE 1. Introduction 2. Complexity 3. Waves in microstructured materials internal variables examples 4. Biophysics / biomechanics 5. Complexity around snow 6. Final remarks 2 One of the most highly
More information3 Balance equations ME338A CONTINUUM MECHANICS
ME338A CONTINUUM MECHANICS lecture otes 1 thursy, may 1, 28 Basic ideas util ow: kiematics, i.e., geeral statemets that characterize deformatio of a material body B without studyig its physical cause ow:
More informationCS 468. Differential Geometry for Computer Science. Lecture 17 Surface Deformation
CS 468 Differential Geometry for Computer Science Lecture 17 Surface Deformation Outline Fundamental theorem of surface geometry. Some terminology: embeddings, isometries, deformations. Curvature flows
More informationMITOCW MITRES2_002S10nonlinear_lec05_300k-mp4
MITOCW MITRES2_002S10nonlinear_lec05_300k-mp4 The following content is provided under a Creative Commons license. Your support will help MIT OpenCourseWare continue to offer high quality educational resources
More informationEngineering Sciences 241 Advanced Elasticity, Spring Distributed Thursday 8 February.
Engineering Sciences 241 Advanced Elasticity, Spring 2001 J. R. Rice Homework Problems / Class Notes Mechanics of finite deformation (list of references at end) Distributed Thursday 8 February. Problems
More informationNon-Linear Finite Element Methods in Solid Mechanics Attilio Frangi, Politecnico di Milano, February 17, 2017, Lesson 5
Non-Linear Finite Element Methods in Solid Mechanics Attilio Frangi, attilio.frangi@polimi.it Politecnico di Milano, February 17, 2017, Lesson 5 1 Politecnico di Milano, February 17, 2017, Lesson 5 2 Outline
More informationChapter 0. Preliminaries. 0.1 Things you should already know
Chapter 0 Preliminaries These notes cover the course MATH45061 (Continuum Mechanics) and are intended to supplement the lectures. The course does not follow any particular text, so you do not need to buy
More informationContinuum Mechanics and Theory of Materials
Peter Haupt Continuum Mechanics and Theory of Materials Translated from German by Joan A. Kurth Second Edition With 91 Figures, Springer Contents Introduction 1 1 Kinematics 7 1. 1 Material Bodies / 7
More informationContinuum Mechanics Fundamentals
Continuum Mechanics Fundamentals James R. Rice, notes for ES 220, 12 November 2009; corrections 9 December 2009 Conserved Quantities Let a conseved quantity have amount F per unit volume. Examples are
More informationFundamentals of Fluid Dynamics: Elementary Viscous Flow
Fundamentals of Fluid Dynamics: Elementary Viscous Flow Introductory Course on Multiphysics Modelling TOMASZ G. ZIELIŃSKI bluebox.ippt.pan.pl/ tzielins/ Institute of Fundamental Technological Research
More informationCVEN 7511 Computational Mechanics of Solids and Structures
CVEN 7511 Computational Mechanics of Solids and Structures Instructor: Kaspar J. Willam Original Version of Class Notes Chishen T. Lin Fall 1990 Chapter 1 Fundamentals of Continuum Mechanics Abstract In
More informationYou may not start to read the questions printed on the subsequent pages until instructed to do so by the Invigilator.
MATHEMATICAL TRIPOS Part III Thursday 1 June 2006 1.30 to 4.30 PAPER 76 NONLINEAR CONTINUUM MECHANICS Attempt FOUR questions. There are SIX questions in total. The questions carry equal weight. STATIONERY
More informationCH.5. BALANCE PRINCIPLES. Multimedia Course on Continuum Mechanics
CH.5. BALANCE PRINCIPLES Multimedia Course on Continuum Mechanics Overview Balance Principles Convective Flux or Flux by Mass Transport Local and Material Derivative of a olume Integral Conservation of
More informationChapter 3. Forces, Momentum & Stress. 3.1 Newtonian mechanics: a very brief résumé
Chapter 3 Forces, Momentum & Stress 3.1 Newtonian mechanics: a very brief résumé In classical Newtonian particle mechanics, particles lumps of matter) only experience acceleration when acted on by external
More informationA CONTINUUM MECHANICS PRIMER
A CONTINUUM MECHANICS PRIMER On Constitutive Theories of Materials I-SHIH LIU Rio de Janeiro Preface In this note, we concern only fundamental concepts of continuum mechanics for the formulation of basic
More informationTraction on the Retina Induced by Saccadic Eye Movements in the Presence of Posterior Vitreous Detachment
Traction on the Retina Induced by Saccadic Eye Movements in the Presence of Posterior Vitreous Detachment Colangeli E., Repetto R., Tatone A. and Testa A. Grenoble, 24 th October 2007 Table of contents
More informationConservation of mass. Continuum Mechanics. Conservation of Momentum. Cauchy s Fundamental Postulate. # f body
Continuum Mechanics We ll stick with the Lagrangian viewpoint for now Let s look at a deformable object World space: points x in the object as we see it Object space (or rest pose): points p in some reference
More informationME338A CONTINUUM MECHANICS
ME338A CONTINUUM MECHANICS lecture notes 10 thursday, february 4th, 2010 Classical continuum mechanics of closed systems in classical closed system continuum mechanics (here), r = 0 and R = 0, such that
More informationFundamentals of Linear Elasticity
Fundamentals of Linear Elasticity Introductory Course on Multiphysics Modelling TOMASZ G. ZIELIŃSKI bluebox.ippt.pan.pl/ tzielins/ Institute of Fundamental Technological Research of the Polish Academy
More informationNon-Classical Continuum Theories for Solid and Fluent Continua. Aaron Joy
Non-Classical Continuum Theories for Solid and Fluent Continua By Aaron Joy Submitted to the graduate degree program in Mechanical Engineering and the Graduate Faculty of the University of Kansas in partial
More informationPOLITECNICO DI MILANO
POLITECNICO DI MILANO MASTER DEGREE THESIS IN MECHANICAL ENGINEERING EXPERIMENTAL INDENTIFICATION OF MATERIAL PROPERTIES OF GELS Thesis supervisor: Prof. Giorgio Previati Name: Xinhao Lu Student ID number:
More informationMultiscale modeling and simulation of shock wave propagation
University of Iowa Iowa Research Online Theses and Dissertations Spring 2013 Multiscale modeling and simulation of shock wave propagation Cory Nelsen University of Iowa Copyright 2013 Cory Nelsen This
More informationAn Atomistic-based Cohesive Zone Model for Quasi-continua
An Atomistic-based Cohesive Zone Model for Quasi-continua By Xiaowei Zeng and Shaofan Li Department of Civil and Environmental Engineering, University of California, Berkeley, CA94720, USA Extended Abstract
More informationThe Finite Element Method II
[ 1 The Finite Element Method II Non-Linear finite element Use of Constitutive Relations Xinghong LIU Phd student 02.11.2007 [ 2 Finite element equilibrium equations: kinematic variables Displacement Strain-displacement
More informationComparison of Models for Finite Plasticity
Comparison of Models for Finite Plasticity A numerical study Patrizio Neff and Christian Wieners California Institute of Technology (Universität Darmstadt) Universität Augsburg (Universität Heidelberg)
More informationDiscrete Analysis for Plate Bending Problems by Using Hybrid-type Penalty Method
131 Bulletin of Research Center for Computing and Multimedia Studies, Hosei University, 21 (2008) Published online (http://hdl.handle.net/10114/1532) Discrete Analysis for Plate Bending Problems by Using
More informationIII.3 Momentum balance: Euler and Navier Stokes equations
32 Fundamental equations of non-relativistic fluid dynamics.3 Momentum balance: Euler and Navier tokes equations For a closed system with total linear momentum P ~ with respect to a given reference frame
More informationLaw of behavior very-rubber band: almost incompressible material
Titre : Loi de comportement hyperélastique : matériau pres[...] Date : 25/09/2013 Page : 1/9 Law of behavior very-rubber band: almost incompressible material Summary: One describes here the formulation
More informationCH.9. CONSTITUTIVE EQUATIONS IN FLUIDS. Multimedia Course on Continuum Mechanics
CH.9. CONSTITUTIVE EQUATIONS IN FLUIDS Multimedia Course on Continuum Mechanics Overview Introduction Fluid Mechanics What is a Fluid? Pressure and Pascal s Law Constitutive Equations in Fluids Fluid Models
More informationNonlinear Equations for Finite-Amplitude Wave Propagation in Fiber-Reinforced Hyperelastic Media
Nonlinear Equations for Finite-Amplitude Wave Propagation in Fiber-Reinforced Hyperelastic Media Alexei F. Cheviakov Department of Mathematics and Statistics, University of Saskatchewan, Saskatoon, Canada
More informationConfigurational Forces as Basic Concepts of Continuum Physics
Morton E. Gurtin Configurational Forces as Basic Concepts of Continuum Physics Springer Contents 1. Introduction 1 a. Background 1 b. Variational definition of configurational forces 2 с Interfacial energy.
More informationKinetics of Particles
Kinetics of Particles A- Force, Mass, and Acceleration Newton s Second Law of Motion: Kinetics is a branch of dynamics that deals with the relationship between the change in motion of a body and the forces
More informationHooke s law and its consequences 1
AOE 354 Hooke s law and its consequences Historically, the notion of elasticity was first announced in 676 by Robert Hooke (635 73) in the form of an anagram, ceiinosssttuv. He explained it in 678 as Ut
More informationNonlinear Waves in Solid Continua with Finite Deformation
Nonlinear Waves in Solid Continua with Finite Deformation by Jason Knight Submitted to the graduate degree program in Department of Mechanical Engineering and the Graduate Faculty of the University of
More informationUniversità degli Studi di Bari. mechanics 1. Load system determination. Joint load. Stress-strain distribution. Biological response 2/45 3/45
Università degli Studi di Bari mechanics 1 Load system determination Joint load Stress-strain distribution Biological response 2/45 3/45 ? 4/45 The human body machine Energy transformation Work development
More informationELAS - Elasticity
Coordinating unit: Teaching unit: Academic year: Degree: ECTS credits: 2017 295 - EEBE - Barcelona East School of Engineering 737 - RMEE - Department of Strength of Materials and Structural Engineering
More informationConstitutive models: Incremental (Hypoelastic) Stress- Strain relations. and
Constitutive models: Incremental (Hypoelastic) Stress- Strain relations Example 5: an incremental relation based on hyperelasticity strain energy density function and 14.11.2007 1 Constitutive models:
More informationRelaxation methods and finite element schemes for the equations of visco-elastodynamics. Chiara Simeoni
Relaxation methods and finite element schemes for the equations of visco-elastodynamics Chiara Simeoni Department of Information Engineering, Computer Science and Mathematics University of L Aquila (Italy)
More information06 - balance equations - open system balance equations. balance equations. balance equations. balance equations. thermodynamic systems
06 - - open systems thermodynamic systems open system thermodynamic system which is allowed to exchange mechanical work, heat and mass, typically, and its environment. enclosed by a deformable, diathermal,
More informationON THE CONSTITUTIVE MODELING OF THERMOPLASTIC PHASE-CHANGE PROBLEMS C. Agelet de Saracibar, M. Cervera & M. Chiumenti ETS Ingenieros de Caminos, Canal
On the Constitutive Modeling of Thermoplastic Phase-change Problems C. AGELET DE SARACIBAR y & M. CERVERA z ETS Ingenieros de Caminos, Canales y Puertos Edificio C1, Campus Norte, UPC, Jordi Girona 1-3,
More informationThis introductory chapter presents some basic concepts of continuum mechanics, symbols and notations for future reference.
Chapter 1 Introduction to Elasticity This introductory chapter presents some basic concepts of continuum mechanics, symbols and notations for future reference. 1.1 Kinematics of finite deformations We
More informationConstitutive Relations
Constitutive Relations Andri Andriyana, Ph.D. Centre de Mise en Forme des Matériaux, CEMEF UMR CNRS 7635 École des Mines de Paris, 06904 Sophia Antipolis, France Spring, 2008 Outline Outline 1 Review of
More informationNDT&E Methods: UT. VJ Technologies CAVITY INSPECTION. Nondestructive Testing & Evaluation TPU Lecture Course 2015/16.
CAVITY INSPECTION NDT&E Methods: UT VJ Technologies NDT&E Methods: UT 6. NDT&E: Introduction to Methods 6.1. Ultrasonic Testing: Basics of Elasto-Dynamics 6.2. Principles of Measurement 6.3. The Pulse-Echo
More informationChapter 6: Momentum Analysis of Flow Systems
Chapter 6: Momentum Analysis of Flow Systems Introduction Fluid flow problems can be analyzed using one of three basic approaches: differential, experimental, and integral (or control volume). In Chap.
More informationChapter 1 Fluid Characteristics
Chapter 1 Fluid Characteristics 1.1 Introduction 1.1.1 Phases Solid increasing increasing spacing and intermolecular liquid latitude of cohesive Fluid gas (vapor) molecular force plasma motion 1.1.2 Fluidity
More informationThe Finite Element Method for the Analysis of Non-Linear and Dynamic Systems. Prof. Dr. Eleni Chatzi Lecture ST1-19 November, 2015
The Finite Element Method for the Analysis of Non-Linear and Dynamic Systems Prof. Dr. Eleni Chatzi Lecture ST1-19 November, 2015 Institute of Structural Engineering Method of Finite Elements II 1 Constitutive
More informationInternational Journal of Pure and Applied Mathematics Volume 58 No ,
International Journal of Pure and Applied Mathematics Volume 58 No. 2 2010, 195-208 A NOTE ON THE LINEARIZED FINITE THEORY OF ELASTICITY Maria Luisa Tonon Department of Mathematics University of Turin
More informationForce, Friction & Gravity Notes
Force, Friction & Gravity Notes Key Terms to Know Speed: The distance traveled by an object within a certain amount of time. Speed = distance/time Velocity: Speed in a given direction Acceleration: The
More informationDifferential relations for fluid flow
Differential relations for fluid flow In this approach, we apply basic conservation laws to an infinitesimally small control volume. The differential approach provides point by point details of a flow
More informationA unified flow theory for viscous fluids
Laboratoire Jacques-Louis Lions, Paris 27/10/2015 A unified flow theory for viscous fluids ILYA PESHKOV CHLOE, University of Pau, France joint work with EVGENIY ROMENSKI Sobolev Institute of Mathematics,
More informationEXPERIENCE COLLEGE BEFORE COLLEGE
Mechanics, Heat, and Sound (PHY302K) College Unit Week Dates Big Ideas Subject Learning Outcomes Assessments Apply algebra, vectors, and trigonometry in context. Employ units in problems. Course Mathematics
More informationNotes 4: Differential Form of the Conservation Equations
Low Speed Aerodynamics Notes 4: Differential Form of the Conservation Equations Deriving Conservation Equations From the Laws of Physics Physical Laws Fluids, being matter, must obey the laws of Physics.
More informationISSUES IN MATHEMATICAL MODELING OF STATIC AND DYNAMIC LIQUEFACTION AS A NON-LOCAL INSTABILITY PROBLEM. Ronaldo I. Borja Stanford University ABSTRACT
ISSUES IN MATHEMATICAL MODELING OF STATIC AND DYNAMIC LIQUEFACTION AS A NON-LOCAL INSTABILITY PROBLEM Ronaldo I. Borja Stanford University ABSTRACT The stress-strain behavior of a saturated loose sand
More informationLinear Constitutive Relations in Isotropic Finite Viscoelasticity
Journal of Elasticity 55: 73 77, 1999. 1999 Kluwer Academic Publishers. Printed in the Netherlands. 73 Linear Constitutive Relations in Isotropic Finite Viscoelasticity R.C. BATRA and JANG-HORNG YU Department
More information03 - introduction to vectors and tensors. me338 - syllabus. introduction tensor calculus. tensor calculus. tensor calculus.
03 - introduction to vectors and tensors me338 - syllabus holzapfel nonlinear solid mechanics [2000], chapter 1.6-1.9, pages 32-55 03-1 introduction 2 tensor the word tensor was introduced in 1846 by william
More informationChapter 6: Momentum Analysis
6-1 Introduction 6-2Newton s Law and Conservation of Momentum 6-3 Choosing a Control Volume 6-4 Forces Acting on a Control Volume 6-5Linear Momentum Equation 6-6 Angular Momentum 6-7 The Second Law of
More informationConstitutive Relations
Constitutive Relations Dr. Andri Andriyana Centre de Mise en Forme des Matériaux, CEMEF UMR CNRS 7635 École des Mines de Paris, 06904 Sophia Antipolis, France Spring, 2008 Outline Outline 1 Review of field
More informationConstitutive models: Incremental plasticity Drücker s postulate
Constitutive models: Incremental plasticity Drücker s postulate if consistency condition associated plastic law, associated plasticity - plastic flow law associated with the limit (loading) surface Prager
More informationNatural States and Symmetry Properties of. Two-Dimensional Ciarlet-Mooney-Rivlin. Nonlinear Constitutive Models
Natural States and Symmetry Properties of Two-Dimensional Ciarlet-Mooney-Rivlin Nonlinear Constitutive Models Alexei Cheviakov, Department of Mathematics and Statistics, Univ. Saskatchewan, Canada Jean-François
More informationRecap. The bigger the exhaust speed, ve, the higher the gain in velocity of the rocket.
Recap Classical rocket propulsion works because of momentum conservation. Exhaust gas ejected from a rocket pushes the rocket forwards, i.e. accelerates it. The bigger the exhaust speed, ve, the higher
More informationOn the Numerical Modelling of Orthotropic Large Strain Elastoplasticity
63 Advances in 63 On the Numerical Modelling of Orthotropic Large Strain Elastoplasticity I. Karsaj, C. Sansour and J. Soric Summary A constitutive model for orthotropic yield function at large strain
More informationCONTINUUM MECHANICS - Nonlinear Elasticity and Its Role in Continuum Theories - Alan Wineman NONLINEAR ELASTICITY AND ITS ROLE IN CONTINUUM THEORIES
CONINUUM MECHANICS - Nonlinear Elasticity and Its Role in Continuum heories - Alan Wineman NONLINEAR ELASICIY AND IS ROLE IN CONINUUM HEORIES Alan Wineman Department of Mechanical Engineering, University
More information4/13/2015. Outlines CHAPTER 12 ELECTRODYNAMICS & RELATIVITY. 1. The special theory of relativity. 2. Relativistic Mechanics
CHAPTER 12 ELECTRODYNAMICS & RELATIVITY Lee Chow Department of Physics University of Central Florida Orlando, FL 32816 Outlines 1. The special theory of relativity 2. Relativistic Mechanics 3. Relativistic
More informationChapter 3 Stress, Strain, Virtual Power and Conservation Principles
Chapter 3 Stress, Strain, irtual Power and Conservation Principles 1 Introduction Stress and strain are key concepts in the analytical characterization of the mechanical state of a solid body. While stress
More informationNewton s Laws of Motion. Chapter 3, Section 2
Newton s Laws of Motion Chapter 3, Section 2 3 Motion and Forces Inertia and Mass Inertia (ih NUR shuh) is the tendency of an object to resist any change in its motion. If an object is moving, it will
More informationQuasistatic Nonlinear Viscoelasticity and Gradient Flows
Quasistatic Nonlinear Viscoelasticity and Gradient Flows Yasemin Şengül University of Coimbra PIRE - OxMOS Workshop on Pattern Formation and Multiscale Phenomena in Materials University of Oxford 26-28
More informationMomentum and Collisions
Momentum and Collisions Vocabulary linear momemtum second law of motion isolated system elastic collision inelastic collision completly inelastic center of mass center of gravity 9-1 Momentum and Its Relation
More informationChapter 11 Rotational Dynamics and Static Equilibrium. Copyright 2010 Pearson Education, Inc.
Chapter 11 Rotational Dynamics and Static Equilibrium Units of Chapter 11 Torque Torque and Angular Acceleration Zero Torque and Static Equilibrium Center of Mass and Balance Dynamic Applications of Torque
More informationStructural Analysis of Truss Structures using Stiffness Matrix. Dr. Nasrellah Hassan Ahmed
Structural Analysis of Truss Structures using Stiffness Matrix Dr. Nasrellah Hassan Ahmed FUNDAMENTAL RELATIONSHIPS FOR STRUCTURAL ANALYSIS In general, there are three types of relationships: Equilibrium
More informationOther state variables include the temperature, θ, and the entropy, S, which are defined below.
Chapter 3 Thermodynamics In order to complete the formulation we need to express the stress tensor T and the heat-flux vector q in terms of other variables. These expressions are known as constitutive
More informationNONLINEAR CONTINUUM FORMULATIONS CONTENTS
NONLINEAR CONTINUUM FORMULATIONS CONTENTS Introduction to nonlinear continuum mechanics Descriptions of motion Measures of stresses and strains Updated and Total Lagrangian formulations Continuum shell
More informationSEMM Mechanics PhD Preliminary Exam Spring Consider a two-dimensional rigid motion, whose displacement field is given by
SEMM Mechanics PhD Preliminary Exam Spring 2014 1. Consider a two-dimensional rigid motion, whose displacement field is given by u(x) = [cos(β)x 1 + sin(β)x 2 X 1 ]e 1 + [ sin(β)x 1 + cos(β)x 2 X 2 ]e
More informationComputational Modelling of Mechanics and Transport in Growing Tissue
Computational Modelling of Mechanics and Transport in Growing Tissue H. Narayanan, K. Garikipati, E. M. Arruda & K. Grosh University of Michigan Eighth U.S. National Congress on Computational Mechanics
More information